摘要:
The invention relates to a method of using a CMOS chip for direct charged particle counting. To avoid reset noise, it is known to use Correlative Double Sampling: for each signal value the pixel is sampled twice: once (204) directly after reset and once (206) after an integration time. The signal is then determined (208) by subtracting the reset value from the later acquired value, and the pixel is reset again (202). Typically the integration time is chosen sufficiently short that the chance that two particles impinge on one pixel is negligible, thereby enabling event counting. Although this technique removes reset noise and fixed pattern noise, it also lowers the image rate to half the frame rate, as a pixel needs to be sampled twice for one signal value. The invention proposes to reset the pixel only after a large number of read-outs. This is based on the insight that typically a large number of events, typically approximately 10, are needed to cause a full pixel. By either resetting after a large number of images, or when one pixel of the image shows a signal above a predetermined value (for example 0.8 x the full-well capacity), the image speed can be almost doubled when compared to the prior art method, using a reset after acquiring a signal.
摘要:
A detector system for a transmission electron microscope includes a first detector for recording a pattern and a second detector for recording a position of a feature of the pattern. The second detector is preferably a position sensitive detector that provides accurate, rapid position information that can be used as feedback to stabilize the position of the pattern on the first detector. In one embodiment, the first detector detects an electron energy loss electron spectrum, and the second detector, positioned behind the first detector and detecting electrons that pass through the first detector, detects the position of the zero-loss peak and adjusts the electron path to stabilize the position of the spectrum on the first detector.
摘要:
In a transmission electron microscope detector system, image data is read out from the pixels and analyzed during an image acquisition period. The image acquisition process is modified depending on the results of the analysis. For example, the analyses may indicate the inclusion in the data of an image artifact, such as charging or bubbling, and data including the artifact may be eliminated form the final image. CMOS detectors provide for selective read out of pixels at high data rates, allowing for real-time adaptive imaging.
摘要:
The invention relates to a method of using a direct electron detector in a TEM, in which an image with a high intensity peak, such as a diffractogram or an EELS spectrum, is imaged on said detector. As known the high intensity peak may damage the detector. To avoid this damage, the centre of the image is moved, as a result of which not one position of the detector is exposed to the high intensity, but the high intensity is smeared over the detector, displacing the high intensity peak before damage results.
摘要:
In a transmission electron microscope detector system, image data is read out from the pixels and analyzed during an image acquisition period. The image acquisition process is modified depending on the results of the analysis. For example, the analyses may indicate the inclusion in the data of an image artifact, such as charging or bubbling, and data including the artifact may be eliminated form the final image. CMOS detectors provide for selective read out of pixels at high data rates, allowing for real-time adaptive imaging.
摘要:
The invention relates to a method of using a CMOS chip for direct charged particle counting. To avoid reset noise, it is known to use Correlative Double Sampling: for each signal value the pixel is sampled twice: once (204) directly after reset and once (206) after an integration time. The signal is then determined (208) by subtracting the reset value from the later acquired value, and the pixel is reset again (202). Typically the integration time is chosen sufficiently short that the chance that two particles impinge on one pixel is negligible, thereby enabling event counting. Although this technique removes reset noise and fixed pattern noise, it also lowers the image rate to half the frame rate, as a pixel needs to be sampled twice for one signal value. The invention proposes to reset the pixel only after a large number of read-outs. This is based on the insight that typically a large number of events, typically approximately 10, are needed to cause a full pixel. By either resetting after a large number of images, or when one pixel of the image shows a signal above a predetermined value (for example 0.8 x the full-well capacity), the image speed can be almost doubled when compared to the prior art method, using a reset after acquiring a signal.
摘要:
In a transmission electron microscope detector system, image data is read out from the pixels and analyzed during an image acquisition period. The image acquisition process is modified depending on the results of the analysis. For example, the analyses may indicate the inclusion in the data of an image artifact, such as charging or bubbling, and data including the artifact may be eliminated form the final image. CMOS detectors provide for selective read out of pixels at high data rates, allowing for real-time adaptive imaging.
摘要:
A method of performing tomographic imaging of a sample in a charged-particle microscope, comprising the following steps: - Providing a beam of charged particles that propagate along a particle-optical axis; - Providing the sample on a sample holder that can be tilted relative to said beam; - In an imaging step, directing the beam through the sample so as to form and capture an image of the sample at an image detector; - Repeating this procedure at each of a series of sample tilts so as to acquire a corresponding set of images; - Mathematically processing images from said set so as to construct a composite image of the sample,
whereby, in said imaging step, a sequence of component images is captured at a corresponding sequence of focus settings. This renders a 3D imaging cube rather than a 2D imaging sheet at a given sample tilt.